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Core electrons Critical mass

The commonly accepted pulsar model is a neutron star of about one solar mass and a radius of the order of ten kilometers. A neutron star consists of a crust, which is about 1 km thick, and a high-density core. In the crust free neutrons and electrons coexist with a lattice of nuclei. The star s core consists mainly of neutrons and a few percents of protons and electrons. The central part of the core may contain some exotic states of matter, such as quark matter or a pion condensate. Inner parts of a neutron star cool up to temperatures 108iT in a few days after the star is formed. These temperatures are less than the critical temperatures Tc for the superfluid phase transitions of neutrons and protons. Thus, the neutrons in the star s crust and the core from a superfluid, while the protons in the core form a superconductor. The rotation of a neutron superfluid is achieved by means of an array of quantized vortices, each carrying a quantum of vorticity... [Pg.45]

The critical core mass required to reach all thermonuclear burning stages is called the Chandrasekhar mass. Its value is about 1.4 M0, but it depends on the mean molecular weight per free electron pe — reflecting the balance between pressure and gravity ... [Pg.37]


See other pages where Core electrons Critical mass is mentioned: [Pg.37]    [Pg.119]    [Pg.334]    [Pg.337]    [Pg.364]    [Pg.63]    [Pg.494]    [Pg.6]    [Pg.330]    [Pg.24]    [Pg.81]    [Pg.364]    [Pg.119]    [Pg.701]   
See also in sourсe #XX -- [ Pg.787 ]




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